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Dispersion Modelling The advectiondiffusion equation

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Advection, diffusion, dispersion mechanisms. Diffusive and dispersive fluxes ... contaminant will move as a result of advection and dispersion ... – PowerPoint PPT presentation

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Title: Dispersion Modelling The advectiondiffusion equation


1
Dispersion ModellingThe advection-diffusion
equation
  • Conservation of mass for a simple box

2
Mass balances
  • input output accumulation
  • Total mass
  • Contaminant
  • Advection, diffusion, dispersion mechanisms

3
Diffusive and dispersive fluxes
4
Diffusive and dispersive fluxes
  • Diffusivity, DAB, is determined by temperature,
    pressure, and molecular properties of A and B
    molecules.
  • Dispersion coefficients Di (or Ki), ix, y, z
  • are determined by flow conditions (velocity,
    intensity, and scale of turbulence) and are
    defined consistently with diffusive fluxes,

5
Diffusive and dispersive fluxes
  • Advective, diffusive and dispersive fluxes are
    additive.
  • In atmospheric transport dispersive flux
    dominates diffusive flux.
  • The relation between advective and dispersive
    flux is case dependent, one or the other may
    dominate in different directions.

6
  • Considering both advective and dispersive fluxes,
    we can get (for the contaminant)
  • Note the positioning of the terms to avoid the
    appearance of negative signs.
  • Since the diffusive and dispersive fluxes are
    defined similarly, if we let Dx represent the sum
    of diffusivity and dispersion coefficient in the
    x direction the equation will represent all three
    processes. As already noted, dispersion
    typically dominates anyway in many environmental
    situations.

7
  • Other process may also be considered
  • Generation within box (emissions)
  • Chemical reaction (production or decay)
  • Surface uptake (plants?)
  • Deposition (wet or dry)

8
  • ci concentration of pollutant i,
  • a function of space (x,y,z) and time (t)
  • u,v,w horizontal and vertical wind speed
    components
  • KX, KY horizontal turbulent diffusion
    coefficients
  • KV vertical turbulent exchange coefficients
  • Ri net rate of production of pollutant i by
    chemical reactions
  • Si emission rate of pollutant i
  • Di net rate of change of pollutant i due to
    surface uptake processes
  • Wi net rate of change of pollutant i due to
    wet deposition

9
Dispersion from a point source
10
Figure 4-1 Wark Warner
  • Gaussian or normal distribution function

11
GAUSSIAN (NORMAL) DISTRIBUTION
12
DOUBLE GAUSSIAN DISTRIBUTION
13
  • Can view the plume two ways
  • as a person standing on the ground
  • - Eulerian space
  • - contaminant will move as a result of advection
    and dispersion
  • 2) as a person moving with the air mass
  • - Lagrangian space
  • - contaminant will move as a result of
    dispersion

14
3 DIMENSIONAL DISPERSION MODELLagrangian
approach to the point source problem
  • Similar to heat conduction equation in 3-d
  • Solution for instantaneous release of X g of
    pollutant at t 0 and x y z 0

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18
Lagrangian solutions to the diffusion equation
19
Eulerian viewpoint for an elevated point source
  • Consider advection in only one direction
  • u wind speed in x direction
  • v w 0
  • Consider a release of Q g/s over a short time
    period ?t at time zero, thus, X Q ?t
  • Let the point of release be at (0, 0, H)
  • At time t, the center of the dispersing puff will
    be at (ut, 0, H)

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21
  • If we wish to consider a continuous emission
    source and evaluate the lateral spreading in the
    y and z directions only, the equation becomes
  •  
  •  
  •  
  • where Q mass emission rate, mass/time
  • u advection velocity, length/time
  • See next slide from de Nevers for derivation

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23
Dispersion coefficients
  • Define dispersion coefficients sy and sz in terms
    of Ky and Kz, u and x

24
2-D STEADY DISPERSION MODEL
  • Solution for windspeed of u m/s and continuous
    release of Q g/s of pollutant at x y 0
    (stack location) and z H (the effective
    stack height)
  • H h ??h
  • h physical stack height, ?
  • ?h plume rise due to buoyancy

25
DISPERSION COEFFICIENTS
  • Ky and Kz approximately proportional to wind
    speed
  • Ky/u and Kz/u approximately constant
  • ?y and ?z should vary approximately with
    x(1/2)
  • Field observations show more complex variation
    (Figures 4.6 and 4.7, Wark, Warner Davis)
  • Wind speed and solar flux combine to give
    stability classes A - F (Table 6.1 de Nevers)

26
  • Horizontal dispersion coefficient

27
  • Vertical dispersion coefficient

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29
Algebraic expressions for dispersion coefficients
  • The graphical representations of ?y and ?z can
    be approximated by algebraic expressions using
    parameters in Tables 4-1 through 4-3 of Wark,
    Warner, and Davis.

30
Algebraic representation of dispersion
coefficients Rural environment
31
Algebraic representation of dispersion
coefficients Urban environment
32
Algebraic representation of dispersion
coefficients Urban environment
33
ATMOSPHERIC TURBULENCE AND SAMPLING TIME
  • The time scale for atmospheric turbulence can be
    quite long, of the order of many minutes.
  • Field observations of dispersion coefficients are
    specific to the sampling (averaging) time used
    (typically 10 minutes)
  • Estimates of corrections for other sampling
    periods can be made

34
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